Abstract

Birds appear to be equipped with a light-dependent, radical-pair-based magnetic compass that relies on truly quantum processes. While the identity of the sensory protein has remained speculative, cryptochrome 4 has recently been identified as the most auspicious candidate. Here, we report on all-atom molecular dynamics (MD) simulations addressing the structural reorganisations that accompany the photoreduction of the flavin cofactor in the European robin cryptochrome 4 (ErCry4). Extensive MD simulations reveal that the photo-activation of ErCry4 induces large-scale conformational changes on short (hundreds of nanoseconds) timescales. Specifically, the photo-reduction is accompanied with the release of the C-terminal tail, structural rearrangements in the vicinity of the FAD-binding site, and the noteworthy formation of an α-helical segment at the N-terminal part. Some of these rearrangements appear to expose potential phosphorylation sites. We describe the conformational dynamics of the protein using a graph-based approach that is informed by the adjacency of residues and the correlation of their local motions. This approach reveals densely coupled reorganisation entities, i.e. graph communities, which could facilitate an efficient signal transduction due to a high density of hubs. These communities are interconnected by a small number of highly important residues. The network approach clearly identifies the sites restructuring upon photo-activation, which appear as protrusions or delicate bridges in the reorganisation network. We also find that, unlike in the homologous cryptochrome from D. melanogaster, the release of the C-terminal domain does not appear to be correlated with the transposition of a histidine residue close to the FAD cofactor.

Highlights

  • Magnetoreception, the remarkable trait of perceiving Earth’s weak magnetic field, is widespread among the animal kingdom [1,2,3,4]

  • The mean Root-mean-square deviations (RMSD) per residue (figure 1(c)) reveals that large RMSDs are accrued at the C-terminal tail (CTT) and, to a lesser extent, several loop regions

  • The largest differences of mean RMSD per residue for the dark state (DS) and RPD state are observed for the CTT and the mobile regions surrounding residues 45, 185 and the region following the C-terminal lid around residue number 410

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Summary

Introduction

Magnetoreception, the remarkable trait of perceiving Earth’s weak magnetic field, is widespread among the animal kingdom [1,2,3,4]. Most notably the compass sense in migratory birds [1, 2, 5,6,7,8], the accumulated evidence supports Schulten’s revolutionary hypothesis of a radical pair-based magnetic sensor [9]. According to this model, magnetoreception is the result of the quantum coherent evolution of the singlet and triplet states of transient pairs of radicals under the influence of spin-selective reactions and magnetic interactions [10]. We focus on the processes that follow up on this initial stage

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